As the Reynold's Number NR depends on density p, average speed v and coefficient ofviscosity I, then let us say. $\text{N}_\text{R}\propto \rho^\text{a}\text{v}^b\eta^\text{c}$
Again is proportional to the diameter of the pipe , combining the two we have
. $\text{N}_\text{R}\propto \rho ^\text{a}\text{v}^\text{b}\eta^\text{c}\text{d}$ $\text{N}_\text{R }= \text{ K} \rho^\text{a} \text{v}^\text{b}\eta^\text{c}\text{d}$
We write ,$[\text{N}_\text{R}]= [\text{M}^0\text{L}^0\text{T}^0]$
$[\rho]= [\text{MK}^{-3}]$
$[\text{v}]= [\text{LT}^{-1}]$
$[\eta] = [ \text{ML}^{-1} \text{T}^{-1}]$
$[\text{d}]= [\text{L}]$
Syubstituting the dimension in (i), we have , $[\text{M}^0\text{L}^0\text{T}] = [\text{ML}^{-3}]^\text{a}[\text{LT}^{-1}]^\text{b}[\text{ML}^{-1}\text{T}^{-1}]^\text{c}[\text{L}]$
$= \text{M}^{(\text{a+c})} \text{L }^{(-3\text{a+b+c+1})}\text{T}^{(\text{-b-c})}$
Comparing the dimensions of M,L and T, we have, $\text{a+c}=0$
$-3\text{a+b-c+1=0}$
$-\text{b}-\text{c} =0$
On simplifying, we get $\text{c}= -1$
$\text{b}=1$
$\text{a}=1$
Therefore, the relation(i) becomes $\text{N}_\text{R} =\text{K}\rho^1 \text{v}^1\eta^{-1}\text{d}$
$\text{N}_\text{R}=\text{K}\rho^1\text{v}^1\eta^{-1}\text{d}$
$\text{N}_\text{R} = \text{K}\rho\frac{\text{vd}}{\eta}$
$\text{N}_\text{R} = \propto\rho\frac{\text{vd}}{\eta}$